Low-Frequency Prototype of Laser Interferometer Suspensions

Low-Frequency Prototype of Laser Interferometer Suspensions
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This presentation explores the development of a low-frequency prototype for laser interferometer suspensions aimed at detecting gravitational waves below 10 Hz. The project focuses on overcoming challenges such as external noise interference and discusses noise reduction techniques using machine-learning algorithms. Detector sensitivity, experimental setups, and noise subtraction methods are also examined in the context of gravitational wave detection in the low-frequency regime.

  • Laser Interferometer
  • Gravitational Waves
  • Noise Reduction
  • Machine Learning
  • Experimental Setups

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  1. Low Frequency Prototype of Laser Interferometer Suspensions for Gravitational Wave Detection Presentation By: Yuka Lin Mentor: Dr. Michele Zanolin (Department of Astronomy & Physics) Embry-Riddle Aeronautical University Acknowledgements: Dr. Darrel Smith (Embry-Riddle Aeronautical University), Dr. Gabriele Vajente (California Institute of Technology), Dr. Anne Boettcher

  2. LIGO = Laser Interferometer Gravitational-Wave Observatory https://www.researchgate.net/figure/Left-panel-LIGO-Hanford-site-USA-The-two-arms-of-the- interferometer-are-about_fig3_331246187 https://arxiv.org/abs/1710.09973

  3. Experimental Model Set-Up Torsion Pendulum Lower Optics Bench Upper Optics Bench

  4. The overall goal of this project: The overall goal of this project: detecting gravitational waves (GW s) in the low frequency regime (below 10 Hz) https://en.wikipedia.org/wiki/Type_II_supernova Essentially, this regime is where the supernovae core-collapse and pre-merger binary star mergers are relevant.

  5. Detector Sensitivity The graph shows the level of strain noise that LIGO detectors can detect. The lower the lines, the more sensitive the detectors are. https://arxiv.org/abs/1604.00439

  6. The Main Problem It is extremely difficult to detect GW s in the low frequency regime since they would be obscured by external noise (i.e. ground vibration) that will interfere with the suspended test masses However, there are methods to possibly reduce the noise

  7. Noise Subtraction Algorithms from machine-learning techniques were created to reduce the non-stationary noise couplings from the detector output. https://arxiv.org/abs/1911.09083

  8. Noise Subtraction ? ? = ?[? ? ] + ?? [??? ?(?)] ?=1 Parameters: (?)= output strain of GW detectors ?(?)and ??(?) = filters (witness channels) ?? = non-stationary noise coupling ? = stationary noise coupling

  9. Example Output for 60 Hz Powerline: The full code for the algorithm: https://git.ligo.org/gabriele-vajente/nonsens

  10. References Martynov, D. V. et al. Sensitivity of the Advanced LIGO Detectors at the Beginning of Gravitational Wave Astronomy. Physical Review D 93.11 (2016): n. pag. Crossref. Web. Type ii supernova. (2021, March 28). Retrieved April 02, 2021, from https://en.wikipedia.org/wiki/Type_II_supernova Vajente, G., Huang, Y., Isi, M., Driggers, J., Kissel, J., Szczepanczyk, M., & Vitale, S. (2020, January 28). Machine-learning non-stationary noise out of gravitational wave detectors. Retrieved April 02, 2021, from https://arxiv.org/abs/1911.09083 Viets, A., Wade, M., Urban, A., Kandhasamy, S., Betzwieser, J., Brown, D., . . . Weinstein, A. (2018, March 13). Reconstructing the calibrated strain signal in the advanced ligo detectors. Retrieved April 02, 2021, from https://arxiv.org/abs/1710.09973

  11. Questions? Contact: liny10@my.erau.edu

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